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Direct, Bending, Torsion stresses and Principal Stresses
Dr.R.Ramesh Professor Department of Mechanical Engineering Sri Venkateswara College of Engineering, Sriperumbudur, chennai
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TYPE OF LOADS AND STRESSES IN REAL- TIME APPLICATIONS
Dead loads Live loads axial (tension- compression) , flexural (bending) torsion(twisting) in nature. Steady loads Variable loads Shock loads (suddenly) Impact loads (applied with some velocity) Thermal Loading
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Static Load Stress Stress Ratio, R = 1.0
F and P are applied and remain constant Stress A static (steady) load is a stationary force or couple (applied to a member) that does not change in magnitude, point of application, and direction. Stress Ratio, R = 1.0 Time
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Dynamic Load: An element subjected to Dynamic loads
(tensile and compressive stresses involved) Continuous total load reversal over time
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Dynamic Load…. Loads that vary during normal service of the product …..& produce dynamic stresses Dynamic stress can be cyclic or random. Parts subject to dynamic stress?
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a) & b) Schematic diagram of Gear train system
c) & d) Schematic diagram of Cone pulley drive for propeller fan
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The design involves Deflection and Rigidity Stress and Strength
(a) Bending deflection (b) Torsional deflection (c) Shear deflection due to transverse loading Stress and Strength (a) Static Strength (b) Fatigue Strength (c) Impact Strength Product Reliability
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Failure Examples Fig. 5–1 Failure of truck driveshaft spline due to corrosion fatigue Shigley’s Mechanical Engineering Design
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Failure Examples Impact failure of a lawn-mower blade driver hub.
Fig. 5–2 Impact failure of a lawn-mower blade driver hub. The blade impacted a surveying pipe marker. Shigley’s Mechanical Engineering Design
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Failure Examples Fig. 5–3 Failure of an overhead-pulley retaining bolt on a weightlifting machine. A manufacturing error caused a gap that forced the bolt to take the entire moment load. Shigley’s Mechanical Engineering Design
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Failure Examples Fig. 5–5 Valve-spring failure caused by spring surge in an oversped engine. The fractures exhibit the classic 45 degree shear failure Shigley’s Mechanical Engineering Design
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Strength Vs Stress Stress is dependent on the load characteristics.
Strength is an inherent property of the material. . Factor of safety = Strength / Stress = S / σ Factor of safety depends on Type of material How controllable are environment conditions Type of loading and the degree of certainty with which the stresses are calculated Type of application Failure can mean a part has separated into two or more pieces; (brittle) has become permanently distorted, thus ruining its geometry; (ductile) has had its function compromised
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Allowable stress . . . While designing a component, it must be ensured that the maximum stress that may be induced during working life, do not exceed a certain safe limit . . Such a safe limiting stress is known as allowable, permissible or design stress
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Tensile Strength : Comparison
Si crystal <100> Graphite/ Ceramics/ Semicond Metals/ Alloys Composites/ fibers Polymers Tensile strength, TS (MPa) PVC Nylon 6,6 10 100 200 300 1000 Al (6061) a ag Cu (71500) hr Ta (pure) Ti Steel (1020) (4140) qt (5Al-2.5Sn) W cw L DPE PP PC PET 20 30 40 2000 3000 5000 Graphite Al oxide Concrete Diamond Glass-soda Si nitride H wood ( fiber) wood(|| fiber) 1 GFRE (|| fiber) ( fiber) C FRE A FRE( fiber) E-glass fib Aramid fib Room Temp. values Based on data in Table B4, Callister 7e. a = annealed hr = hot rolled ag = aged cd = cold drawn cw = cold worked qt = quenched & tempered AFRE, GFRE, & CFRE = aramid, glass, & carbon fiber-reinforced epoxy composites, with 60 vol% fibers.
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Mechanical Properties
Slope of stress strain plot (which is proportional to the elastic modulus) depends on bond strength of metal
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TENSILE STRESS: When a body is subjected to two equal and
opposite axial pulling forces, F - F as shown in Fig. the stress induced at any section A – A of the body is known as tensile stress and the corresponding strain, the tensile strain (the ratio of total elongation, 8 to the original length, l).
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COMPRESSIVE STRESS: When a body is subjected to two equal and opposite axial pushing forces, F
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SHEAR STRESS: Single shearing of a riveted joint. When a body is subjected to two equal and opposite forces acting tangentially across the resisting section, as a result of which the body tends to shear off the section, then the stress induced is called shear stress.
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the area resisting the shear off the rivet
Double shearing of a riveted joint.
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Bearing Stress A localised compressive stress at the surface of
contact between two members of a machine part, that are relatively at rest is known as bearing stress or crushing stress. the bearing stress or crushing stress (stress at the surface of contact between the rivet and a plate
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Torsional Shear Stress
When a machine member is subjected to the action of two equal and opposite couples acting in parallel planes (or torque or twisting moment), then the machine member is said to be subjected to torsion.
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Consider a straight beam subjected to a bending moment M
as shown in Fig. The bending equation is given by
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Load and stress analysis:
A footstep to design Static strength
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Load and stress analysis:
A footstep to design Static strength PRINCIPAL STRESSES / PLANES Analytical approach
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plane-stress transformation equations
2D –General Stress State plane-stress transformation equations
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1 2 Equation (1) defines two particular values for the angle 2φp,
the maximum normal stress σ1 and the other, the minimum normal stress σ2. These two stresses are called the principal stresses, The angle between the principal directions is 90°. 2 Equation (2) defines the two values of 2φs at which the shear stress τ reaches an extreme value. The angle between the surfaces containing the maximum shear stresses is 90°
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Determination of principal and shear stresses
Formulas for the two principal stresses can be obtained by The two extreme-value of shear stresses are found to be
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Using Mohr’s circle, finding the principal stresses and directions: graphical approach
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Failure Theories – Static Loads
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